Abstract

We consider the thermodynamics of a square Ising lattice which is constructed from unit cells of height $n$ lattice spacings and width $m$ lattice spacings. In a particular unit cell the values of the $2mn$ exchange energies can be chosen at will. Once specified this basic unit cell is repeated to make up the entire planar lattice. For arbitrary $n$ and for $m=2$ and $m=3$ we obtain the exact equations for the critical point. Furthermore, we show that when $n$ is finite and $m=1$ or $m=2$ the specific heat has a singularity of the form $A\mathrm{ln}|1\ensuremath{-}\frac{T}{{T}_{c}}|$ and we derive an explicit formula for $A$. Our method can be extended to values of $mg2$. A numerical evaluation of our results shows that the average of $A$ over impurity configurations is smaller for $m=1$ than for $m=2$.

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